A parameter was added for the unloading return stress, F eSA , to appr translation - A parameter was added for the unloading return stress, F eSA , to appr Chinese Traditional how to say

A parameter was added for the unloa

A parameter was added for the unloading return stress, F e
SA , to approximate the unloading
path after large strain excursions. A parameter was also added to incorporate residual strain into
the hysteretic model, R STFact . It was found that the magnitude of residual strain for the behavior
shown in Figure 3a was approximately proportional to the cumulative dissipated energy with a
residual strain factor computed to be R STFact =0.00721 (%/MPa-m/m). The ability of the hysteretic
model to capture the cyclic response of SMA rod is demonstrated in Figure 4b using parameters,
E SMA =28,650 MPa, F s
AS =308 MPa, R s =0.033E SMA , d f
AS =0.0412 m/m, R m =0.30E SMA , F f
SA =221 MPa,
F e
SA =124 MPa, and R STFact =0.00721 %/MPa. The experimental response is plotted without the
initial R-phase shown in Figure 4b because it is assumed that this portion of response will already
be expended as the rod is pretensioned to an initial stress above the R-phase plateau. It is shown
that the model is capable of approximately simulating the unloading path and residual stresses
upon unloading.
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Results (Chinese Traditional) 1: [Copy]
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為卸載返回應力,F e 添加參數SA,近似的卸載大應變遊覽後的路徑。此外增加了一個參數,納入到殘餘應變滯回模型,R STFact。它被發現的殘餘應變大小的行為顯示在圖 3a 是近似成正比與累積消耗的能量殘餘應變因數計算應 R STFact = 0.00721 (%/MPa-m/m)。滯回的能力模型以捕獲 SMA 杆的迴圈回應表明圖 4b 中使用的參數,E SMA = 28,650 m p a,F s= 308 MPa,R s = 0.033E SMA,機組如 = 0.0412 m/m,R m = 0.30E SMA,F fSA = 221 MPa,F eSA = 124 MPa 和 R STFact = 0.00721%/MPa。實驗回應繪製沒有初始的 R 相圖 4b 中所示,因為它假設,這部分的反應已經將支用杆先張法預應力與初始應力水準以上研發階段高原。它是所示該模型是能夠近似地類比卸荷的路徑及殘餘應力在卸載。
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Results (Chinese Traditional) 2:[Copy]
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一個參數用於卸載回報的壓力,女ê加入
SA,近似卸載
大應變遊覽後的路徑。的參數也被加入到將殘餘應變進入
遲滯模式,R STFact。已經發現,殘餘應變為行為的幅度
在圖3a所示為大致成比例的累積耗散能量與
計算為R = STFact 0.00721(%/兆帕-米/米)殘餘應變因子。遲滯的能力
模型捕捉SMA棒的循環反應是表現在圖4b中使用參數
,êSMA = 28650兆帕,Fs的
AS = 308兆帕,R S = 0.033E SMA,DF
AS =0.0412米/平方米, R M = 0.30E SMA,量F f
SA = 221兆帕
,˚FêSA
= 124兆帕,而R STFact = 0.00721%/兆帕。實驗響應標繪而不
因為假定響應的該部分將已經在圖4b所示的初始R相
被消耗的棒預緊到R相高原以上的初始應力。它表明
,該模型能夠大致模擬卸載路徑和殘餘應力
時卸載。
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Results (Chinese Traditional) 3:[Copy]
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卸載返回應力,f,近似卸載的路徑後,大應變遊覽的參數。一個參數也被納入到
殘餘應變滯回模型,R stfact。發現殘餘應變值的大小為行為
如圖3a所示是累積消耗的能量與
近似成正比殘餘應變因數計算是R stfact = 0.00721(% / m / m)。
的滯回模型捕捉SMA杆迴圈反應的能力是在圖4b中使用參數顯示,
E SMA = 28650 MPa,F的
= 308 MPa,R = 0.033e SMA,D F
= 0.0412 / M,R M = 0.30e SMA,F
SA = 221 MPa,
F E
SA = 124 MPa,與R stfact = 0.00721% / MPa。實驗反應繪製無圖4b所示
初始R是因為它認為這部分的反應已經
花費為杆預應力的初始應力比R高原。所示的模型是能够近似類比卸載路徑和卸載後的殘餘應力。
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